A NNALES DE L ’I. H. P., SECTION C
K EWEI Z HANG
Quasiconvex functions, SO(n) and two elastic wells
Annales de l’I. H. P., section C, tome 14, n
o6 (1997), p. 759-785
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Quasiconvex functions, SO(n) and two elastic wells
Kewei ZHANG Ann. Inst Henri Poincaré,
Vol. 14, n° 6, 1997, p. 759-785 Analyse non linéaire
School of Mathematics, Physics, Computing and electronics, Macquarie University, NSW 2109, Australia.
E-mail: [email protected]
ABSTRACT. - We use
approximations
ofminimizing
sequences tostudy
thegrowth
of somequasiconvex
functions near their zero sets.We show that for
SO(n) ,
thequasiconvexification
of the distance functionSO (n) )
can be bounded belowby
the distance function itself. In certain cases of theincompatible
two elastic well structure, we establisha similar result. We also prove that for small
Lipschitz perturbations
ofSO(n)
and of the two well structure, theYoung
measure limits ofgradients supported
on theseperturbed
sets are Dirac masses.1. INTRODUCTION
The
study
ofYoung
measures limit ofgradients [KP, BFJK] supported
in various
compact
sets inMN n and quasiconvex
relaxations of certain distance functions to these sets are veryimportant subjects
in thestudy
ofmartensitic
phase
transitions andoptimal design problems (see [CK, BJl, BJ2, F, K, KS]).
As far as Iknow, explicit
relaxation formulas are hard to obtain and there areonly
a few knownexamples [Dal, Da2, KS, K, D2, DR]. Therefore,
thestudy
of the behaviour ofquasiconvex
functions is very difficult because we cannot work on themdirectly.
It isclosely
related tothe
analysis
ofquasiconvex
hulls of theneighbourhoods
of the zero sets forgiven non-negative
functions and thestability problems
related toYoung
Annales de l’Institut Henri Poincaré - Analyse non lineaire - 0294-1449 Vol. 14/97/06/@ Elsevier, Paris
760 K. ZHANG
measures under
perturbations.
In this paper, wegive
someexamples
wherewe can estimate the
growth
of certainquasiconvex
functions of the formfor some closed subset K C where is the space of all N x n real
matrices,
withoutknowing
the exact formula ofF(P),
andwhere
Qdistp (P, K)
is thequasiconvexification
ofdistp (P, K),
and p > l.We establish these results for
SO(n)
and for twoincompatible
elasticwells
SO(n)
USO(n)H
when H satisfies the technical condition(1.3)
below. The
p-th
power of a distance function to agiven compact
set is thesimplest
function fromgeometric point
of view and thequasiconvex
relaxations of this
type
of functionsgive
information ofquasiconvex
hullsof the
neighbourhoods
of the zero sets of theoriginal
functions.The main results are the
following.
THEOREM 1.1. -
Suppose n 2:
2. LetF(P)
=Qdist2(P, SO(n))
be the
quasiconvexification (cf. [Da 1, Da2],
also seeDefinition 2.1 ) of
dist2(P, SO(n)),
P E Mnxn. Then there exists a constantc(n)
>0,
suchthat
for all
P EThe method we use for
proving
of Theorem 1.1applies
to twoincompatible
elastic wells under a further technical condition. Let n > 3 andwhere
SO(n)H
={RH, R E SO (n) ~,
and H is a n x npositive
definitediagonal
matrixsatisfying
It was
proved
in[Ma, Sv]
that thequasiconvex
hull of K definedby (1.2)
remains K itself underassumption (1.3).
Wehave,
COROLLARY 1.2. -
Suppose n 2 3,
K isgiven by (1.2)
with Hsatisfying (1.3). Then,
there exists apositive
constantc(n, H)
> 0 such thatWe also
study
theYoung
measure limit ofgradients ([KP, BFJK]) supported
’near’SO(n)
andSO(n)
USO(n)H.
Wegive
some estimateslinéaire
QUASICONVEX FUNCTIONS, SO(n) AND TWO ELASTIC WELLS 761
of the
quasiconvex
hull of theE-neighbourhood
of these sets. Thisproblem
is related to the
stability
of ’one-well’ and twoincompatible
well structurewhen n = 3. For a
compact
set K CMNxn,
letand let be the
quasiconvex
hull ofKa
for a > 0. We haveCOROLLARY 1.3. - Assume
(1.3).
There exist constantsC(n)
>0, C(n, H)
>0,
such thatand
for
all E > 0.We
always
assume that H c IRn is a bounded open and connected set with smoothboundary.
Letf : SO(n) -~
Mn"nand g : SO(n)
Ube
Lipschitz
functions such thatfor some E > 0.
We have
THEOREM 1.4. -
Suppose
thatf
and g aredefined
asabove,
letK f
andKg
be theirgraphs, respectively,
i.e.Let be a bounded sequence in 1 p ~, such that u~ ~ u in and
dist(Duj, I~ f ) -~
0(dist(Duj, K9 ) -~ 0,
respectively)
almosteverywhere as j
~ ~.Then, for sufficiently
smallE > 0 and up to a
subsequence,
Du almosteverywhere.
In otherwords, Kf
andIg
supportonly
trivialYoung
measure limitof gradients (see
Theorem 2.4for
thedefinition of Young measures).
Similar to Theorem
l.l,
we haveCOROLLARY 1.5. -
Suppose
that n >2,
and letf
and gsatisfy ( 1.5)
and(1.6), respectively, for
E > 0sufficiently
small. LetF(P)
=Qdist2(P, Kf),
Vol. 14, nO 6-1997.
762 K.ZHANG
and let
G(P)
=Qdist2(P,kg)
be thequasiconvexifications of dist2 (P, K f)
and
dist2(P, respectively.
Then there exists a constantc(n, E)
> 0such that
for
all P EThe methods we use to prove Theorem 1.1 are:
(i)
anapproximation
ofW 1 ~ 2 minimizing
sequencesby YT~ l ~‘~
sequences(Lemma 3.1), using
themaximal function method
through
a modified version of[Z,
Lemma3.1];
(ii)
V.Sverak’s
idea ofshowing
that a sequence is aCauchy
sequence[Sv].
To prove Theorem 1.1 and
Corollary 1.2,
we have to make use of thespecial
structure of the sets
concerned,
thatis,
bothSO(n)
andSO(n)
USO(n)H
have the
property
for some a >
0,
whereadjP
is thetranspose
of the cofactors of P E Mnxn(see [Sv]).
In order to use thisproperty,
the sequences understudy
should bein at least. When n >
3,
our sequence is bounded intherefore,
we have to
approximate
theoriginal
sequenceby
a bounded sequence inWl°°.
I do not known how tobypass
Lemma 3.1 and prove the resultdirectly.
Theapproximation
lemma(Lemma 3.1)
stands on its ownright.
It
gives
an estimate of the minimum energy ofquasiconvex
relaxations for distance functionsdistp ( ~, K)
forgeneral compact
sets K cM N x n
whenwe
only
minimize the energy on a set of bounded functions.In
§2,
notation andpreliminaries
aregiven
which will be used to prove our main results.§3
is devoted toestablishing
theapproximation
lemma which is crucial to theproof
of Theorem 1.1. In§4,
we prove the results stated above.To conclude this
section,
wejustify
that the functiondist2 (P, SO (n) )
isnot
quasiconvex
itself. Infact,
it is not trivial to prove it.PROPOSITION 1.6. -
,S’O (n) ) : quasiconvex.
Proof. -
Letf (P) = min~~P - A12, ~P -
whereA,
B Eare fixed matrices. It was established in
[K]
that thequasiconvexification
Q f
off
has theexplicit
formQUASICONVEX FUNCTIONS, WO(n) AND TWO ELASTIC WELLS 763
where is the
greatest eigenvalue
of the matrix(A - B)T (A - B).
Now, set .4 =
7,
B = .J, where I is the n x ii,identity matrix,
where 12
andI" _~~
are 2 x 2 and(7z - 2)
x(n - 2) identity
matricesrespectively.
ConsiderF(P) = I ~2, ~P -
P EMnxn,
wehave
F(P) > ,5’C)(71,)),
since~,
J ESO(n).
IfSO(n))
was
quasiconvex, by
Definition 2.2below, QF(P) > dist2(P, SO(n)),
forevery P E 1’tI " X " . In
particular, QF(0) > dist2(0, SO(n) ),
where 0 is then x zero matrix. We have
and if we notice that = 4 when A =
I,
B =J,
we haveContradiction. The
proof
iscomplete.
02. NOTATION AND PRELIMINARIES
Throughout
the rest of this.paper 0
is a bounded open subset of IRn. We denoteby
the space of real N x n matrices with theIRNn metric;
hence the norm of P E is defined
by I
P~_
wheretr is the trace
operator
andPT
is thetranspose
of P. The innerproduct
of two matrices in
MNxn
is P.Q
=trPTQ.
For an n x n matrixP,
denote
by adjP
thetranspose
of the cofactors of P.SO ( n)
is the set ofall rotations with determinant 1. For a
compact
subset K CMNxn,
letconvK,
diamK be the convexhull,
diameter and the norm ofK, respectively,
whereWe write for the space of continuous functions
(~ : ~ 2014~
!Rhaving compact support
in0,
and define =C 1 ( SZ )
n IfVol. 14, n° 6-1997.
764 K. ZHANG
1 p
cxJ we denoteby LP(03A9;RN)
the Banach space ofmappings
u : Q - u =
(ui , ... , u_; ) ,
such that uz eLP (Q)
for eachI,
with norm> =
~N i=1 ~ui~Lp(03A9). Similarly,
we denoteby
theusual Sobolev space of
mappings
u eLP (Q ; R°" )
all of whose distributionalderivatives ~ui ~xj = Djui, I
I N, I j
n, belong
to LP(Q).
W ,P (Q, R )
is a Banach space under the normwhere Du = and we
define,
asusual, f~l’~ )
to be theclosure of
f~ l’~ )
in thetopology
ofWeak and weak * convergence of sequences are written as ~ and
-~,
respectively.
If H C P eMNxn,
then we write H + P to denotethe
set {P
+Q : Q
eH ~ , j H = ~ j x,
x eH ~
for aninteger j
> 0. Wedefine the distant function for a set K C
by
DEFINITION 2.1.
(see Morrey
BallBall,
Currie and Olver(BCOJ). -
A continuousfunction f :
isquasiconvex if
for
every P E ECo ( U;
and every open bounded subset U cFor a
given function,
we can consider itsquasiconvexification
(quasiconvex relaxation):
,DEFINITION 2.2.
(see Dacorogna Suppose f :
I~ is acontinuous
function.
Thequasiconvexification of f
isdefined by
and will be denoted denoted
by Q f.
PROPOSITION 2.3.
(see Dacorogna (DaJ). - Suppose f :
(~ iscontinuous,
thenwhere SZ c is a bounded domain. In
particular
thein fimum
in(2.1 )
isindependent of
the choiceof
Q.Annales de l’Institut Henri Poincaré - linéaire
QUASICONVEX FUNCTIONS, SO(rt) AND TWO ELASTIC WELLS 765
We use the
following
theoremconcerning
the existence andproperties
of
Young
measures from Tartar[T].
For results in a moregeneral
contextand their
proofs,
the reader is referred to Berliocchi andLasry [BL],
Balder[Bd]
and Ball[B 13 ] .
THEOREM 2.4. - Let
(z~~~ )
be a bounded sequence inL°° (SZ;
Thenthere exist a
subsequence (z~v> )
anda family of probability
measures on
~s, depending measurably
on x ESZ,
such thatfor
every continuousfunction f :
I~s -~ (~.We say that vx is a trivial
Young
measure at x E H if v~ for someA e
IRs, where 8 A
is the Dirac mass at A.Suppose
that H C Rn. Afamily
ofparametrized measures {vx}x~03A9
iscalled a
Young
measure limit ofgradients [BFJK, KP],
if it isgenerated by
a sequence ofgradients Duj
with bounded inW1,p(03A9,RN).
Let r > 0 and x
E Rn,
setB(x, r) = {y
eIRn :1 y - x r~
andmeas(B(x, r))
= where is the area of the n -1 dimensionalsphere.
DEFINITION 2.5.
(The
MaximalFunction). -
Let u ECo (Rn ).
Wedefine
where we set
for
everylocally
summablef.
LEMMA 2.7.
Vol. 14, n ° 6-1997.
766 K. ZHANG
for
all x E R". Moreover(see [20]) if
p >1,
thenand
if
p >1,
thenfor
all A > 0.LEMMA 2.8.
Then
for
every x, y EH03BB
we haveLEMMA 2.9. - Let X be a metric space, E a
subspace of X,
and k apositive
real number. Then anyk-Lipschitz mapping from
E into (~ can beextended to a
k-Lipschitz mapping from
X into I~.For the
proof
see[ET,
page298].
DEFINITION 2.10.
(see
page234J). -
Let SZ C I~n be open. Let B c f~p be a Borel subset. Amapping
is said to be a
Carathéodory function if
( 1 ) for
almost all x ES2, ~ (x, . )
is continuous onB, (2) for
all a EB, f(., a)
is measurable on SZ.We will not introduce the more
general
notion of normalintegrals
towhich the Measurable Selection Theorem
applies (see [ET,
page234]).
THEOREM 2.1 l.
(The
measurable selection theorem(see (ET,
page236J).
- Let B be a compact subset
of
Rp and g aCarathéodory function of
03A9 x B.Then,
there exists a measurablemapping
ic : SZ --~ B such thatfor
all x E SZ:Annales de l’Institut Henri Poincaré - Analyse linéaire
767 QUASICONVEX FUNCTIONS, SO(n) AND TWO ELASTIC WELLS
A direct consequence of Theorem 2.11 is the
following:
PROPOSITION 2.12. - Let B c I~p be a compact subset and let u : SZ --~ I~P be an
integrable mapping.
Then there exists a measurablemapping
ic : B such that
for
all x E SZWe conclude this section
by giving
the definition ofquasiconvex
hullQK
of acompact
set K CMNxn,
and somesimple properties
of it. Weuse a more restricted definition than that in
[S].
DEFINITION 2.13.
(see
Let K CMN"n
be non-empty and compact.The
quasiconvex
hullQK of
K isdefined by
PROPOSITION 2.14.
and
It is easy to see that is
quasiconvex, QK
Cf a f (0)
andQK
=We may assume that
f ~ f (0)
iscompact, otherwise,
take theconvex function
which is the
squared
distance function to a convex set. Therefore+ g
isquasiconvex.
We claim that(fa!
+ CconvK,
hence it iscompact.
This is easy to see because
fa f
> 0 and = convK. Wehave,
forany fixed 1 p oo,
From
[Z,
Theorem1.1]
and itsproof,
we see that for acompact
zero setfa f (0) corresponding
to anonnegative quasiconvex
function and for any1 ~
p oo,Hence, Ki
cfa f (0))
for everyquasiconvex
functionf,
thusK1
cQK.
The
proof
iscomplete.
DVo!.14,n° 6-1997.
768 K. ZHANG
3. THE APPROXIMATING LEMMA
In this section we establish our main
approximation
lemma whichapplies
to
general compact
sets inLEMMA 3.1. -
Suppose
that K C is a compact subset. Let 1 p oc. Let P EMNxn be
such thatthat
is,
where D =
(0, 1)n
C ~n is the unit cube. Then there exist aminimizing
sequence bounded in such that
~c~ - 0 in a bounded sequence
(gj)
in anda constant
C(n, N, p)
such thatwhere r~~ ~ 0
as j
~ oo,and
Proof - Let 03C6j
ECo (D,
be aminimizing
sequenceas j
~ ~, where ~j ~ 0 is anonnegative
sequence. LetKp
={A 2014 P,
A ~
~C},
and set769 QUASICONVEX FUNCTIONS, SO(n) AND TWO ELASTIC WELLS
It is easy to see that
We have
as j -
oo. SinceKp is compact,
we see that is bounded inWo ’p ( D, (~ N ) ;
infact,
sincewe have
Extend ~~
to be defined in IRn as aperiodic function,
and then letfor j
=1, 2, ... ,
and xED. It is easy to see that is bounded in and up to asubsequence,
~c~ ~ 0 in LetB(o,11)
be a ball inMN n
such thatKp
CB(o,11)
and2-(p-1)p
>Extend ~c~
by
zero outsideD,
we see that u~ E(~ ~’T )
uj =
(u(1)j,..., u(N)j).
For eachfixed j, i,
defineLemma 2.8 ensures that for all x, y e
H~ ,
Let be a
Lipschitz
functionextending
outsideHI
withLipschitz
constant not
greater
thanC(n)A (Lemma 2.9).
SinceHI
is an open set,we have
Vol. 14, n 6-1997.
770 K. ZHANG
for all x E
H~
andIf
H~ _ ~,
set 0 for x E D. IfHI
nD ~ ~,
then we mayalso assume that
Indeed, fixing y
EH;
nD,
for every x ED,
where we have used Lemma 2.7 to assert
that u~2 ~ ( g ) ~ ( M * u~.2 ) ) ( g )
Awhen y e
H~ .
Now set( g~ 1 ~ , ... , g~ N ~ ) .
In order to estimate
J D Kp)dx,
we start from theinequality
and find a bound for
meas ( D ~ H~ ) .
Similar to the
proof
of Lemma 3.1 in[Z],
wehave,
from the definition ofand
Define h :
by
Annales de l’lnstitut Henri Poincaré -
QUASICONVEX FUNCTIONS, SO(n) AND TWO ELASTIC WELLS 771
so that we can prove that
In
fact,
when >2 ,
we have a sequence of a~ >0,
0 and a sequence of balls
Bk
=B(x, Rk)
such thatwhich
implies
Passing
to the limit A; ~ oo in(3.6),
we obtain(3.5) (we
have chosen~> A).
From Lemma
2.6,
we haveAlso,
from Lemma2.6, together
with theembedding theorem,
we haveVol. 14, n° 6-1997.
772 K. ZHANG
as j
-~ oe. ThereforeSince ~~
isperiodic,
we haveTherefore,
which
implies
thatFrom the above two sets of
inequalities,
we haveHence
Annales de l’Institut Henri Poincaré - linéaire
QUASICONVEX FUNCTIONS, AND TWO ELASTIC WELLS 773
Consequently,
Hence,
Also,
fromwe deduce that
thus,
Therefore
Vol. n v 6-1997.
774 K. ZHANG
Given
A,
B eMNxn,
if we takeQ
EKp
such that =dist ( A, Kp ),
we have
and so
Therefore,
from(3.11)
we obtainNow, taking
A = = we havewhich
yields (3.3)
afterletting j
-~ oo. Alsoalmost
everywhere
in D andSince
distp(P,convK)
is a convex function anddistp
(P, K),
wehave,
from the definition ofquasiconvexification,
Annales de l’Institut Henri Poincaré -
QUASICONVEX FUNCTIONS, S’O(n) AND TWO ELASTIC WELLS 775
Therefore,
thus,
From the numerical
analysis point
ofview,
when we minimize the energy in a bounded subset ofW 1 ~ °°
and compare the minimum with theminimum,
we haveproved
thefollowing
resultCOROLLARY 3.2. -
Suppose
that K C iscompact.
Then there existCi(n, N, p)
>0, C2 (n, N, p)
>0,
such thatThe
only
fact in thisCorollary
to be remarked is that theW 1 ~ °°
boundof g depends
onK),
while in(3 .15 )
itdepends
on Infact, they
areequivalent
because of thefollowing inequalities,
Remark 3 .1. - From the construction
of gj
in theproof
of Lemma3.1,
we see that even if a
minimizing
sequence is not bounded in wemay find a
W1,~-sequence
such that near the zeropoints
ofQdistp(., K),
it serves as an
approximate minimizing
sequence.4. PROOFS OF THE MAIN RESULTS
Proof of
Theorem 1 .1 . - LetF(P) _ ,S’O (n) )
for P EIt is known
(see [Z])
thatF-1(0) _ SO(n) .
Let 0 a =F(P)
for someP,
i. e.Vol. 14, n° 6-1997.
776 K. ZHANG
By
Lemma3.1,
we find and(gj ) satisfying (3.1)-(3.15)
with p = 2.We have that
and
by (3.15)
We may assume
that,
up to asubsequence,
inFrom the measurable selection theorem
(see Proposition 2.13),
for eachi =
1,2,...,
there exists a measurablemapping Pi :
D -~SO(n),
suchthat
almost
everywhere
in D. LetFollowing Sverak [S],
we consider theintegral
for
2, j
=1, 2,....
From the weakcontinuity property
ofnull-Lagrangians [B I,R],
if we let i -~ oc ,then j
-~ oo,Now,
sinceP2(x), Pj(x)
ESO(n)
almosteverywhere,
we havewhere
adjPi
+ is theexpansion
ofadj (Pj
+nj),
andAnnales de l’Institut Henri Poincaré - linéaire
QUASICONVEX FUNCTIONS, ,SO(n) AND TWO ELASTIC WELLS 777 We then have
Here we have used the facts that
if P, Q E SO(n),
aba2-~- 4 .o
for real numbers and that =P + Dgi.
From
(4.3)
weget
where
C(n)
> 0 is a constantdepending only
on n.Since a~/~ +
Vol. 14, n° 6-1997.
778 K. ZHANG and so, from
(4.4)
and(4.1)
we conclude thatNow we find a lower bound of
Recalling
the estimate(3.11)
onDui|pdx,
wehave,
for ourchoice of
A,
andA,
where ~j =
0, limi~~
~i =0,
andC(n, N, p) _ C(n),
N = n,p = 2 is a
positive
constant.Combining (4.5)
and(4.6),
we see thatSince the
integral
on the left hand side of(4.7)
islower-semicontinuous
asz ~ oc
and ui
-- 0 inR"), letting
z ~ oo we haveAnnales de l’Institut Henri Poincaré - Analyse linéaire
QUASICONVEX FUNCTIONS, SO(n) AND TWO ELASTIC WELLS 779
By applying
the measurable selection lemma(Theorem 2.13)
to the functionQ ~ for Q
ESO (n),
we can find a measurablemapping Qj :
S~ -~SO(n),
such thatfor almost every x E S~. Therefore the
following inequalities
hold almosteverywhere,
and also
As Uj
is aminimizing
sequence, we pass to the limitas j
-~ oo andwe obtain
Since we also have
and when
~P~
> we obtainwhile,
when we havewe conclude that
Vol. 14, n° 6-1997.
780 K. ZHANG
which, together
with(4.10) yields
for some
C(n)
> 0. Therefore we conclude that there existsc(n)
> 0(in
fact
c(n)
=I/C(n))
such thatfor all P e Mnxn. D
Proof of Corollary
1 .2. - In theproof
of Theorem 1.1 we used the fact that ifP, Q
ESO(n),
It was observed
by Sverak
in[Sv] (also
see[Ma])
that under the condition(1.2),
there exists ana(H)
>0,
such thatWe denote
by
thegreatest eigenvalue
of Handwe see that if
P, Q
ESO(n), (4.11 )
holds for a = l. IfP, Q
ESO(n)H,
.
(4.11)
holds for a = This is because we can write P =PIH, Q
=QIH
for someP1, Qi
ESO(n)
and notice that H is adiagonal matrix,
so thatwhile
Hence we reach the conclusion.
Finally,
if P ESO(n)H
andQ
ESO(n),
then we write P =
RH,
where R eS‘ O ( n ),
and since trRH ~trH,
trH R e
SO(n)
and H is adiagonal
matrix withpositive entries,
we see that
QUASICONVEX FUNCTIONS, SO(n) AND TWO ELASTIC WELLS 781 Since
it is clear that
(4.11)
is satisfiedsetting
Take
and
(4.11)
holds for allP, Q
E K. We may follow theproof
of Theorem 1.1 to proveCorollary
1.2. Theonly place
in theproof
of Theorem 1.1 wherea(H)
is involved is the lastinequality (4.3).
Also the constantsC(n), c(n)
in Theorem 1.1 are
replaced by C ( n , H )
andc ( n, H ) , respectively.
DRemark 4.1. - In fact Matos
[Ma] proved
that if for someeigenvalue A/,
ofH,
we havethen the
quasiconvex
hull of K remains itself. It turns outthat,
it isenough
to assume this condition in
Corollary
1.2. What we need is a variation of(4.11 ).
LetEE
=(eij)
be a matrix such that eij = 0 if i~ j,
eii = E forsome E > 0
sufficiently
small if i~
k and ekk = 1. We consider the formThen this form is still a null
Lagrangian.
We alsohave,
for P ESO(n)H, Q
ESO(n),
when E > 0 is small
enough.
Therefore the conclusion ofCorollary
1.2 isstill true under this weaker condition.
Proof of Corollary
1.3. - LetF(P)
=Qdist2(P, SO(n)),
and letP E Then
by proposition
2.15 we haveVol. 14, n° 6-1997.
782 K. ZHANG
and since
using
Theorem 1.1 we obtainThe
proof
isfinished
forSO(n).
The other case is similar. 0Proof of
Theorem 1.4. - Weonly give
aproof
forf :
The
proof for g
is similar. is afamily
ofYoung
measure limit ofgradients supported on K j.
If we can show that v~ is trivial for almost everyx, the
proof
will befinished.
It is known[Z, KP]
that if aYoung
measurelimit of
gradients
hasbounded support,
then theYoung
measure can begenerated by
a bounded sequence inW 1 ~ °° .
Next we notice that if E is smallenough,
then themapping
Y = X +f(X)
fromSO(n)
toKj
isinvertible
and the inverse is continuous. Let
Q(.) :
: SZ --~ Mn x n be measurable. Ifwe
apply
the measurable selectiontheorem,
we may find a measurablemapping
P : SZ --~Kj,
such that/P(x) -
Tdist(Q(x), Kj),
whereP(x)
=R(x)
+f(R(x)),
and R : SZ -~SO(n)
is measurable.Now,
let be a bounded sequence in such that theYoung
measuresgenerated by (Duj)
issupported
inK f
and Uj-~ ~c
inW 1 ~ °° ( S~, (~=’~ ) .
Foreach
j,
we may find a measurablemapping Rj : SO(n)
such thatalmost
everywhere. Let nj
=Rj(x) - f(Rj(x)).
As in theproof
of Theorem
1.1, setting
we have
limi~~ limi~~ Iij
= 0. We also haveAnnales de l’Institut Henri Poincaré - Analyse non linéaire
QUASICONVEX FUNCTIONS, SO(n) AND TWO ELASTIC WELLS 783
where
C(Rj, f(Rj), nj)
is definedby
theexpansion
of the determinantsTherefore we
have,
due to the fact thatRj
E~S’O(n)
andf
satisfies(1.5),
that
Since
Duj = Rj
+f(Rj)
+ nj, from(1.5),
and if we choose E1/2,
we have
Thus we
have,
Vol. 14, n° 6-1997.
784 K. ZHANG
Obviously,
Choosing
E =min~l/2,1/(4~’(n))~,
we see that if we combine(4.13)
and
(4.14),
we haveSince
I
-~0, when j --~
0 in for any p >1,
and(Duj)
isbounded in
L°°, passing
to the limit in i --~ oo, andusing
the fact that the functional on the left hand side of(4.15)
is lowersemicontinuous,
thenletting j
-~ oc in(4.15),
we see thatTherefore vz =
bD.t~ ~ ~~
almosteverywhere.
The
proof
forK~
is similar. DThe
proof
forCorollary
1.5 is similar to that for Theorem 1.1 and it is left to the reader.ACKNOWLEDGEMENTS
This work is
supported by
the Australiangovernment through
theAustralian Research Council. The author would thank the referee for many
helpful suggestions.
[AF] E. ACERBI and N. Fusco, Semicontinuity problems in the calculus of variations, Arch.
Rational Mech. Anal., Vol. 86, 1984, pp. 125-145.
[Bd] E. J. BALDER, A general approach to lower semicontinuity and lower closure in optimal
control theory, SIAM J. Control and Optimization, Vol. 22, 1984, pp. 570-597.
[BL] H. BERLIOCCHI and J. M. LASRY, Intégrandes normales et mesures paramétrées en calcul
des variations, Bull. Soc. Math. France, Vol. 101, pp. 129-184.
[Bl1] J. M. BALL, Convexity conditions and existence theorems in nonlinear elasticity, Arch.
Rational Mech. Anal., Vol. 63, 1977, pp. 337-403.
[Bl2] J. M. BALL, Constitutive inequalities and existence theorems in nonlinear elasticity, in
"Nonlinear Analysis and Mechanics: Heriot - Watt Symposium." Vol. 1 (edited by
R. mJ. Knops), Pitman, London, 1977.
785 [Bl3] J. M. BALL, A version of the fundamental theorem of Young measures, in Partial Differential Equations and Continuum Models of Phase Transitions, (edited by M.
Rascle, D. Serre and M. Slemrod), 1989, 207-215, Springer-Verlag.
[BCO] J. M. BALL, J. C. CURRIE and P. J. OLVER, Null Lagrangians, weak continuity, and
variational problems of arbitrary order, J. Functional Anal., Vol. 41, 1981, pp.
135-174.
[BFJK] K. BHATTACHARYA, N. B. FIROOZY, R. D. JAMES and R. V. KOHN, Restrictions on
Microstructures, Proc. Royal Soc. Edinburgh A Vol. 124, 1994, pp. 843-878 [BJ1] J. M. BALL and R. D. JAMES, Fine phase mixtures as minimizers of energy, Arch.
Rational Mech. Anal., Vol. 100, 1987, pp. 13-52.
[BJ2] J. M. BALL and R. D. JAMES; Proposed experimental tests of a theory of fine
microstructures and the two-well problem, Phil. Royal Soc. Lon., Vol. 338A, 1992, pp. 389-450.
[CK] M. CHIPOT and D. KINDERLEHRER, Equilibrium configurations of crystals, Arch. Rational Mech. Anal., Vol. 103, 1988, pp. 237-277.
[Da1] B. DACOROGNA, Weak Continuity and Weak Lower Semicontinuity of Nonlinear Functionals, Lectures Notes in Math., Springer-Verlag, Berlin, Vol. 922, 1980.
[Da2] B. DACOROGNA, Direct Methods in the Calculus of Variations, Springer, 1989.
[DR] H. LE DRET and A. RAOULT, Enveloppe quasi-convexe de la densité d’énergie de Saint Venant-Kirchhoff, C. R. Acad. Sci. Paris, Série I, Vol. 318, 1994, pp. 93-98.
[ET] I. EKELAND and R. TEMAM, Convex Aanlysis and Variational Problems, North-Holland, 976.
[F] I. FONSECA, The lower quasiconvex envelope of the stored energy function for an elastic
crystal, J. Math. Pures et Appl., Vol. 67, 1988, pp. 175-195.
[K] R. V. KOHN, The relaxation of a double-well energy, Cont. Mech. Therm., Vol. 3, 1991, pp. 981-1000.
[KP] D. KINDERLEHRER and P. PEDREGAL, Characterizations of Young measures generated by gradients, Arch. Rational Mech. Anal., Vol. 115, 1991, pp. 329-365.
[KS] R. V. KOHN and D. STRANG, Optimal design and relaxation of variational problems I, II, III, Comm. Pure Appl. Math., Vol. 39, 1986, pp. 113-137, 139-182, 353-377.
[L] F. C. LIU, A Luzin type property of Sobolev functions, Ind. Univ. Math. J., Vol. 26, 1977, pp. 645-651.
[Ma] J. MATOS, Young measures and the absence of fine microstructures in the 03B1 2014 03B2 quarts phase transition, preprint.
[Mo] C. B. Jr MORREY, Multiple integrals in the calculus of variations, Springer, 1966.
[Sv] V. SVERÁK, On the problem of two wells, preprint.
[St] E. M. STEIN, Singular Integrals and Differentiability Properties of Functions, Princeton University Press, Princeton , 1970.
[T] L. TARTAR, Compensated compactness and applications to partial differential equations,
Nonlinear Analysis and Mechanics: Heriot-Watt Symposium (edited by R. J. Knops)
Vol. IV, 1979, pp. 136-212.
[Z] K.-W. ZHANG, A construction of quasiconvex functions with linear growth at infinity,
Ann. Sc. Norm Sup. Pisa, Serie IV, Vol. XIX, 1992, pp. 313-326.
(Manuscript received October 2, 1995;
revised February 5, 1996. )
Vol. 14, n" 6-1997.